Near-UV to mid-IR reflectance imaging spectroscopy of paintings on the macroscale.

Broad spectral range reflectance imaging spectroscopy (BR-RIS) from the near UV through the mid-infrared (IR) (350 to 25,000 nm or 28,571 to 400 cm-1) was investigated as an imaging modality to provide maps of organic and inorganic artists' materials in paintings. While visible-to-near-IR (NIR) reflectance and elemental x-ray fluorescence (XRF) imaging spectroscopies have been used for in situ mapping, each method alone is insufficient for robust identification. Combining the two improves results but requires complex data processing. To test BR-RIS, image cubes from early Italian Renaissance illuminated manuscripts were acquired using two spectrometers. Maps of pigments, including trace minerals associated with mined azurite, and their associated binding media were made. BR-RIS has a more straightforward analysis approach as implemented here than visible-to-NIR, mid-IR, or XRF imaging spectroscopy alone and offers the largest amount of macroscale information for mapping artists' materials by comparison.

Reducing the flexibility of retinal restores a wild-type-like photocycle in bacteriorhodopsin mutants defective in protein-retinal coupling.

The thermal re-isomerization of retinal from the 13-cis to the all-trans state is a key step in the final stages of the photocycle of the light-driven proton pump, bacteriorhodopsin. This step is greatly slowed upon replacement of Leu-93, a residue in van der Waals contact with retinal. The most likely role of this key interaction is that it restricts the flexibility of retinal. To test this hypothesis, we have exchanged native retinal in Leu-93 mutants with bridged retinal analogs that render retinal less flexible by restricting free rotation around either the C10-C11 (9,11-bridged retinal) or C12-C13 (11,13-bridged retinal) single bonds. The effect of the analogs on the photocycle was then determined spectroscopically by taking advantage of the previous finding that the decay of the O intermediate in the Leu-93 mutants provides a convenient marker for retinal re-isomerization. Time-resolved spectroscopic studies showed that both retinal analogs resulted in a dramatic acceleration of the photocycling time by increasing the rate of decay of the O intermediate. In particular, exchange of native retinal in the Leu-93 --> Ala mutant with the 9,11-bridged retinal resulted in an acceleration of the decay of the O intermediate to a rate similar to that seen in wild-type bacteriorhodopsin. We conclude that the protein-induced restriction of conformational flexibility in retinal is a key structural requirement for efficient protein-retinal coupling in the bacteriorhodopsin photocycle.

The residues Leu 93 and Asp 96 act independently in the bacteriorhodopsin photocycle: studies with the leu 93-->Ala, Asp 96-->Asn double mutant.

Previous mutagenesis studies with bacteriorhodopsin have shown that reprotonation of the Schiff's base is the rate-limiting step in the photocycle of the D96N mutant, whereas retinal re-isomerization and return of the protein to the initial state constitute the rate-limiting events in the photocycle of the L93A mutant. Thus, in the D96N mutant, decay of the M intermediate is slowed down by more than 100-fold at pH 7. In the L93A mutant, decay of the O intermediate is slowed down by 250-fold. We report here that in the L93A, D96N double mutant, decay of the M intermediate, as well as the formation and decay of the O intermediate, are slowed down dramatically. The photocycle is completed by the decay of a long-lived O intermediate, as in the L93A mutant. The decay of the M and O intermediates in the double mutant parallels the behavior seen in the single mutants over a wide temperature and pH range, arguing that the observed independence is an intrinsic property of the mutant. The slow decay of the M and O intermediates can be selectively and independently reversed under conditions identical to those used for the corresponding intermediates in the D96N and L93A single mutants. Because the effects of the two individual mutations are preserved in the double mutant and can be independently reversed, we conclude that residues Asp 96 and Leu 93 act independently and at different stages of the bacteriorhodopsin photocycle. These results also show that formation of the O intermediate only requires protonation of the Schiff's base and is independent of the protonation of Asp 96 from the aqueous medium.

Molecular mechanism of protein-retinal coupling in bacteriorhodopsin.

Bacteriorhodopsin is a membrane protein that functions as a light-driven proton pump. Each cycle of proton transport is initiated by the light-induced isomerization of retinal from the all-trans to 13-cis configuration and is completed by the protein-driven reisomerization of retinal to the all-trans configuration. Previous studies have shown that replacement of Leu-93, a residue in close proximity to the 13-methyl group of retinal, by alanine, resulted in a 250-fold increase in the time required to complete each photocycle. Here, we show that the kinetic defect in the photocycle of the Leu-93-->Ala mutant occurs at a stage after the completion of proton transport and can be overcome in the presence of strong background illumination. Time-resolved retinal-extraction experiments demonstrate the continued presence of a 13-cis intermediate in the photocycle of the Leu-93-->Ala mutant well after the completion of proton release and uptake. These results indicate that retinal reisomerization is kinetically the rate-limiting step in the photocycle of this mutant and that the slow thermal reisomerization can be bypassed by the absorption of a second photon. The effects observed for the Leu-93-->Ala mutant are not observed upon replacement of any other residue in van der Waals contact with retinal or upon replacement of Leu-93 by valine. We conclude that the contact between Leu-93 and the 13-methyl group of retinal plays a key role in controlling the rate of protein conformational changes associated with retinal reisomerization and return of the protein to the initial state.

Primary picosecond molecular events in the photoreaction of the BR5.12 artificial bacteriorhodopsin pigment.

The picosecond dynamics of the photoreaction of an artificial bacteriorhodopsin (BR) pigment containing a retinal in which a five-membered ring spans the C-12 to C-14 positions of the polyene chain (BR5.12) is examined by using time-resolved absorption and fluorescence and resonance Raman spectroscopy. The ring within the retinal chromophore of BR5.12 blocks the C-13 = C-14 isomerization proposed to be a primary step in the energy storage/transduction mechanism in the BR photocycle. Relative to the native BR pigment (BR-570), the absorption spectrum of BR5.12 is red-shifted by 8 nm. The fluorescence spectrum of BR5.12 closely resembles that of BR-570 although the relative fluorescence yield is higher (approximately 10-fold). Picosecond transient absorption (4-ps pulses, 568-662 nm) measurements reveal an intermediate absorbing to the red side of BR5.12. Kinetic fits show that the red-absorbing intermediate appears within < 3 ps and decays with a time constant of 17 +/- 1 ps to form only BR5.12. No emission in the 650- to 900-nm region can be attributed to the red-absorbing species. Since rotation around C-12 - C-13 and isomerization around C-13 = C-14 are prevented in BR5.12, these results demonstrate that motion in these regions of the retinal is (i) necessary to form the K-like intermediate observed in the native BR-570 photocycle and (ii) not necessary to form a red-absorbing intermediate that has spectral and kinetic properties analogous to those of J-625 in the native BR photocycle. Discussions of the excited and ground electronic state assignments for the intermediate observed in the BR5.12 photoreaction are presented.

Picosecond time-resolved absorption and fluorescence dynamics in the artificial bacteriorhodopsin pigment BR6.11.

The picosecond molecular dynamics in an artificial bacteriorhodopsin (BR) pigment containing a structurally modified all-trans retinal chromphore with a six-membered ring bridging the C11=C12-C13 positions (BR6.11) are measured by picosecond transient absorption and picosecond time-resolved fluorescence spectroscopy. Time-dependent intensity and spectral changes in absorption in the 570-650-nm region are monitored for delays as long as 5 ns after the 7-ps, 573-nm excitation of BR6.11. Two intermediates, J6.11 and K6.11/1, both with enhanced absorption to the red (> 600 nm) of the BR6.11 spectrum are observed within approximately 50 ps. The J6.11 intermediate decays with a time constant of 12 +/- 3 ps to form K6.11/1. The K6.11/1 intermediate decays with an approximately 100-ps time constant to form a third intermediate, K6.11/2, which is observed through diminished 650-nm absorption (relative to that of K6.11/1). No other transient absorption changes are found during the remainder of the initial 5-ns period of the BR6.11 photoreaction. Fluorescence in the 650-900-nm region is observed from BR6.11, K6.11/1, and K6.11/2, but no emission assignable to J6.11 is found. The BR6.11 fluroescence spectrum has a approximately 725-nm maximum which is blue-shifted by approximately 15 nm relative to that of native BR-570 and is 4.2 +/- 1.5 times larger in intensity (same sample optical density). No differences in the profile of the fluorescence spectra of BR6.11 and the intermediates K6.11/1 and K6.11/2 are observed. Following ground-state depletion of the BR6.11 population, the time-resolved fluroescence intensity monitored at 725 nm increases with two time constants, 12 +/- 3 and approximately 100 ps, both of which correlate well with changes in the picosecond transient absorption data. The resonance Raman spectrum of ground-state BR6.11, measured with low-energy, 560-nm excitation, is significantly different from the spectrum of native BR-570, thus confirming that the picosecond transient absorption and picosecond time resolved fluorescence data are assignable to BR6.11 and its photoreaction alone and not to BR-570 reformed during there constitution process (<5% of the BR6.11 sample could be attributed to native BR-570).The J6.11 and K6.11 absorption and fluorescence data presented here are generally analogous to those measured for native J-625 and K-590, respectively, and therefore, the primary events in the BR6.11 photoreaction can be correlated with those in the native BR photocycle. The BR6.11 photoreaction, however, exhibits important differences including slower formation rates for J and K intermediates as well as the presence of a second K intermediate. These results demonstrate that the restricted motion in the C11=C12-C13 region of retinal found in BR6.11 does not greatly change the overall photoreaction mechanism,but does alter the rates at which processes occur.

Time-resolved absorption and fluorescence from the bacteriorhodopsin photocycle in the nanosecond time regime.

Picosecond transient absorption (PTA) in the 568-660-nm region is measured over the initial 80 ns of the bacteriorhodopsin photocycle. After photocycle initiation with 573-nm excitation (7-ps pulsewidth), these PTA data reflect the formation during the initial 40 ps of two long-recognized intermediates with red-shifted (relative to that of BR-570) absorption bands, namely J-625 and K-590. PTA signals at 568, 628, and 652 nm are unchanged for the remainder of the 80-ns photocycle interval measured, demonstrating that no other intermediates, including the proposed KL, are observable by absorption changes. Picosecond time-resolved fluorescence (PTRF), measured at 740 nm, is initiated by 7 ps excitation of the species present at various time delays after the photocycle begins. PTRF signals change rapidly over the initial 40 ps, reflecting, first, the depletion of the ground state BR-570 population and, subsequently, the formation of K-590. The PTRF signal then decreases monotonically with a time constant of 5.5 +/- 0.5 ns from its maximum near a 50-ps delay until it reaches a minimum at a delay of approximately 13 ns. For time delays between 13 and 80 ns, the PTRF signal remains unchanged and slightly higher than that measured from BR-570 alone. The rapid decrease in PTRF signals over the same photocycle interval in which the PTA signals remain unchanged suggests that the retinal-protein interactions involving electronically excited K-590 (K*) are being significantly altered.

Photophysical properties of Sn-porphyrins: potential clinical implications.

The photophysical properties of Sn-protoporphyrin and two of its synthetic analogues, Sn-mesoporphyrin and Sn-diiododeuteroporphyrin, were examined. All three compounds are potent competitive inhibitors of heme oxygenase, the rate-limiting enzyme in the catabolism of heme to bilirubin, and can suppress completely or diminish significantly experimentally induced or naturally occurring forms of jaundice in animals or man. The results of these studies show that all three compounds have long-lived triplet states which are quenched by molecular oxygen both in solution and when incorporated in liposomes. However, the addition of quenching groups such as iodine to the porphyrin macrocycle results in a marked (approximately 60%) decrease in the triplet yield and a threefold decrease in the triplet lifetime. The triplet yield was shown to be independent of the excitation wavelength, and as a result, the metalloporphyrins were extremely poor photosensitizers when excited in the spectral region commonly used in phototherapy. In the presence of serum albumin, the triplet state of Sn-protoporphyrin was not quenched by oxygen. These results indicate that Sn-porphyrins can be custom designed with considerably reduced photosensitizing properties for potential clinical use as inhibitors of bilirubin production.